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Sr$_{0.9}$K$_{0.1}$Zn$_{1.8}$Mn$_{0.2}$As$_{2}$: a ferromagnetic semiconductor with colossal magnetoresistance

机译:sr $ _ {0.9} $ K $ _ {0.1} $ Zn $ _ {1.8} $ mn $ _ {0.2} $ as $ _ {2} $:铁磁性   具有巨大磁阻的半导体

摘要

A bulk diluted magnetic semiconductor (Sr,K)(Zn,Mn)$_{2}$As$_{2}$ wassynthesized with decoupled charge and spin doping. It has a hexagonalCaAl$_{2}$Si$_{2}$-type structure with the (Zn,Mn)$_{2}$As$_{2}$ layer forminga honeycomb-like network. Magnetization measurements show that the sampleundergoes a ferromagnetic transition with a Curie temperature of 12 K and\revision{magnetic moment reaches about 1.5 $\mu_{B}$/Mn under $\mu_0H$ = 5 Tand $T$ = 2 K}. Surprisingly, a colossal negative magnetoresistance, defined as$[\rho(H)-\rho(0)]/\rho(0)$, up to $-$38\% under a low field of $\mu_0H$ = 0.1T and to $-$99.8\% under $\mu_0H$ = 5 T, was observed at $T$ = 2 K. Thecolossal magnetoresistance can be explained based on the Anderson localizationtheory.
机译:通过解耦电荷和自旋掺杂合成了大块稀释的磁性半导体(Sr,K)(Zn,Mn)$ _ {2} $ As $ _ {2} $。它具有六角形的CaAl $ _ {2} $ Si $ _ {2} $型结构,具有(Zn,Mn)$ _ {2} $ As $ _ {2} $层,形成蜂窝状网络。磁化测量表明,样品经历了居里温度为12 K的铁磁跃迁,并且在$ \ mu_0H $ = 5 Tand $ T $ = 2 K}的情况下磁矩达到约1.5 $ \ mu_ {B} $ / Mn。令人惊讶的是,一个巨大的负磁阻定义为$ [\ rho(H)-\ rho(0)] / \ rho(0)$,在$ \ mu_0H $ = 0.1T的低场下高达$-$ 38 \%在$ T $ = 2 K下观察到在$ \ mu_0H $ = 5 T下达到$-$ 99.8 \%。巨大的磁阻可以基于安德森定位理论来解释。

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